2014
DOI: 10.1016/j.aop.2013.10.016
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Zero modes in the light-front coupled-cluster method

Abstract: The light-front coupled-cluster (LFCC) method is a technique for solving Hamiltonian eigenvalue problems in light-front-quantized field theories. Its primary purpose is to provide a systematic sequence of solvable approximations to the original eigenvalue problem without the truncation of Fock space. Here we discuss the incorporation of zero modes, modes of zero longitudinal momentum, into the formalism of the method. Without zero modes, the light-front vacuum is trivial, and the vacuum expectation value of th… Show more

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Cited by 9 publications
(8 citation statements)
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“…Zero modes can be included in the LFCC method [118]. The vacuum must then also be computed as a nontrivial eigenstate, which takes the form of a generalized coherent state of zero modes [64,119].…”
Section: Light-front Coupled-cluster Methodsmentioning
confidence: 99%
“…Zero modes can be included in the LFCC method [118]. The vacuum must then also be computed as a nontrivial eigenstate, which takes the form of a generalized coherent state of zero modes [64,119].…”
Section: Light-front Coupled-cluster Methodsmentioning
confidence: 99%
“…This approach has been applied to a light-front analog of the Greenberg-Schweber model [4,8], where the lowest-order T produces the exact answer, and to QED [7], in a calculation of the dressed-electron state and its anomalous magnetic moment. In addition, a technique for including zero modes has been developed [9] and applied to φ 3 and φ 4 theories and to the Wick-Cutkosky model. Much of this work is less briefly summarized in various proceedings [10][11][12].…”
Section: Overview Of the Methodsmentioning
confidence: 99%
“…However, the original development of the LFCC method did not explicitly include the zero momentum modes needed for representation of a nontrivial light-front vacuum. Here we summarize recent work that rectifies this deficiency [2].…”
Section: Introductionmentioning
confidence: 99%
“…Z maintains the normalization. The eigenvalue problem can then be rewritten as 2) with P − ≡ e −T P − e T an effective Hamiltonian. We project the eigenvalue problem onto the valence and orthogonal sectors 3) with P v the projection onto the valence sector.…”
Section: Introductionmentioning
confidence: 99%
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